+ All Categories
Home > Documents > Puzzler 1 Imagine that you have three boxes, one containing two black marbles, one containing two...

Puzzler 1 Imagine that you have three boxes, one containing two black marbles, one containing two...

Date post: 27-Dec-2015
Category:
Upload: henry-blake
View: 229 times
Download: 1 times
Share this document with a friend
Popular Tags:
14
Puzzler 1 Imagine that you have three boxes, one containing two black marbles, one containing two white marbles, and the third, one black marble and one white marble. The boxes were labeled for their contents – BB, WW and BW – but someone has switched the labels so that every box is now incorrectly labeled . You are allowed to take one marble at a time out of any box, without looking inside, and by this process of sampling you are to determine the contents of all three boxes. What is the smallest number of drawings needed to do this?
Transcript

1

Puzzler

Imagine that you have three boxes, one containing two black marbles, one containing two white marbles, and the third, one black marble and one white marble. The boxes were labeled for their contents – BB, WW and BW – but someone has switched the labels so that every box is now incorrectly labeled. You are allowed to take one marble at a time out of any box, without looking inside, and by this process of sampling you are to determine the contents of all three boxes. What is the smallest number of drawings needed to do this?

2

Solution: One !!!

The key is that every box is incorrectly labeled.

Draw a marble from the box labeled BW

Assume it is black. – you now know which box has 2 black marbles.

Therefore you know the contents of the box labeled WW must be BW (it can’t be labeled correctly!)

Then the third box labeled BB must hold WW marbles

3

Introduction to Audio and Music Engineering

Lecture 7

• Sound waves

• Sound localization

• Sound pressure level

• Range of human hearing

• Sound intensity and power

Period:

Frequency:

Angular Frequency: :Spatial Wavelength

Spatial:Wavenumber

Waves in Space and Time

TSeconds

Hertz (cycles per second)Radians per secondMetersRadians per meter

On a string the frequency of oscillation and the wavelength are connected through the speed of propagation of a bending wave.

c

5

Sound wavesSound is a Longitudinal Wave: Disturbance varies along the direction of propagation.

Transverse wave: (string) Disturbance varies in a direction perpendicular to the direction of propagation.

pres

sure

c = 343 m/sec

Density of air = 1.21 kg/m3

f ≈ 20 Hz 20 kHz

6

Question

What is the wavelength of a sound wave of frequency 20 Hz?

c = 343 m/sec

17.15 meters

c = 343 m/sec = 1125 ft/sec about 1 foot per millisecond

Remember this!

Wavelength = 1.715 cm @ 20 kHz

20 Hz ≤ f ≤ 20 kHz

17 m ≤ ≤ 1.7 cm

7

Human ability to localize sound

Distance between human ears is ≈ 22 – 24 cm

f ≈ 1430 Hz

8

Sound localizationf < 1500 Hz f > 1500 Hz

Wavelength is larger than distance between ears

Wavelength is smaller than distance between ears

Interaural Time Difference (ITD)

Interaural Intensity Difference (IID)

f < 1500 Hz f > 1500 Hz

Humans determine directionality of sound by two basic methods:

But there is some overlap of methods in the range 800:1600 Hz

9

IID and ITD

IID: f ≤ 1500 Hz

Head shadows the sound at more distant ear.

ITD: f ≥ 1500 Hz

ITD time delay:22 cm 650 µsec

The shape of the outer ear (pinna) plays a significant role in 3D audio;Head Related Transfer Function: HRTF

10

Sound Pressure Level

P is the measured pressurePref = 20 µPa (micro-Pascals)

1 Pascal = 1 Newton/meter2

1 Atmosphere = 14.7 lbs/in2 = 1.01 x 105 Pascals

Sound pressure of 20 µPa 0 dB SPL

Sound pressure of 20 Pa 120 dB SPL

1 Atmosphere = 194 dB SPL

11

Range of Human Hearing

HOG ≈ 143 dB

12

Adaptation of Human Hearing

At any given time we hear over a dynamic range of about 90 dB. Our auditory system adapts our hearing sensitivity to the average SPL – much like our eye adjusts to different lighting conditions.

0 dB SPL 140 dB SPL

90 dB

13

Sound Intensity and Power

Sound Intensity: When a pressure wave propagates through air the air moves slightly.

p

u

I = p x u

Dimensional Analysis

Densityof air

Speed of sound

“Impedance” of airSmall air moves a lot

Large air moves little

So … Sound Intensity ≈ Pressure2

14

Inverse Square Law

Power = I x 4πr2

pop

r

I = Power / 4πr2

Total Radiated Sound Power of Musical

InstrumentsEntire Orchestra ≈ 75 WattsTrombone ≈ 6 watts

Violin ≈ 0.1 W


Recommended